Method for light ray steering

ABSTRACT

Techniques and assemblies for light ray steering are described. A method includes receiving solar rays onto a surface of an electro-optic prism. The electro-optic prism includes a first electrode positioned on a first substrate, a second electrode positioned on a second substrate, and an electro-optic material positioned between the first and second electrodes. The first electrode includes multiple substantially parallel linear electrodes. The method further includes applying multiple voltages to some or all of the substantially parallel linear electrodes to generate a refractive index gradient across the electro-optic prism. The method further includes controlling the refractive index gradient so that the solar rays exit the electro-optic prism in a direction substantially normal to a light focusing element, and utilizing the light focusing element to focus the solar rays on a solar energy collector.

CROSS REFERENCE TO RELATED APPLICATIONS

This application claims priority to pending: U.S. ProvisionalApplication Ser. No. 60/752,386, entitled “Prismatic Alignment ofSunlight for Solar Concentrators,” filed on Dec. 22, 2005; U.S.Provisional Application Ser. No. 60/778,918, entitled “Dynamic Steeringof Light Rays by Electro-Optic and Opto-Mechanic Means,” filed on Mar.6, 2006; and U.S. Provisional Application Ser. No. 60/797,691, entitled“Dynamic Steering of Light Rays by Electro-Optic and Opto-MechanicMeans,” filed on May 5, 2006; the entire contents of which above threeprovisional applications are hereby incorporated by reference.

TECHNICAL FIELD

This invention generally relates to techniques and assemblies forsteering light rays.

BACKGROUND

Focusing light rays emanating from either a natural or an artificialsource can be useful for various different applications. For example,steering solar rays to direct them toward a photovoltaic cell or todirect them toward a light focusing element, which then focuses thesolar rays on a photovoltaic cell, can be useful in solar energycollection applications. Generally, a photovoltaic cell (or other devicefor capturing solar energy) is a device that captures solar radiationand converts the radiation into electric potential or current. Aconventional photovoltaic cell is typically configured as a flatsubstrate supporting an absorbing layer, which captures impinging solarradiation, and electrodes, or conducting layers, which serve totransport electrical charges created within the cell.

A solar concentrator is a light focusing element that can be employed tomultiply the amount of sunlight, i.e., the solar flux, impinging on aphotovoltaic cell. A solar energy collection assembly, or array, can bemounted on a moveable platform, in an attempt to keep the absorbinglayer directed approximately normal to the solar rays as the sun tracksthe sky over the course of a day. If a light focusing element, such as alens or curved mirror, is included in the solar energy collectionassembly to focus the solar rays toward the photovoltaic cells, theassembly's position can be adjusted in an attempt to keep the receivingsurface of the light focusing element directed approximately normal tothe solar rays. The platform can be moved manually or automatically bymechanical means, and various techniques can be employed to track thesun.

In general, light rays refract upon passing through a triangular prismat a fixed angle that depends on the prism apex angle, wavelength oflight, the refractive index of the prism material, and the incidentangle of the light rays, assuming the light rays are not totallyinternally reflected inside the prism. A prism used together with alayer of liquid crystal positioned between two contiguous electrodes,such as that described in U.S. Pat. No. 6,958,868, can refract light ofa given wavelength at many different angles, because the refractiveindex of the liquid crystal layer can be varied by varying the strengthof electrical field across the layer. The refractive angle of the lightrays, as they pass through the prism assembly, can therefore becontrolled within some limitations by varying the applied electricfield, thereby steering the light rays within some angular range. Asolar energy collection assembly employing such a prism assembly tosteer solar rays toward a light focusing element is described in U.S.Pat. No. 6,958,868.

SUMMARY

This invention relates to techniques and assemblies for light raysteering. In general, in one aspect, the invention features a methodincluding receiving solar rays onto a surface of an electro-optic prism.The electro-optic prism includes a first electrode positioned on a firstsubstrate, a second electrode positioned on a second substrate, and anelectro-optic material positioned between the first and secondelectrodes. The first electrode includes multiple substantially parallellinear electrodes. The method further includes applying multiplevoltages to some or all of the substantially parallel linear electrodesto generate a refractive index gradient across the electro-optic prism.The method further includes controlling the refractive index gradient sothat the solar rays exit the electro-optic prism in a directionsubstantially normal to a light focusing element, and utilizing thelight focusing element to focus the solar rays on a solar energycollector.

Implementations of the invention can include one or more of thefollowing features. The solar energy collector can include aphotovoltaic device. In one example, the electro-optic material can be aliquid crystal material, e.g., a cholesteric or a nematic liquidcrystal. The electro-optic material positioned between the electrodescan have a substantially uniform thickness. In an embodiment, the methodcan further include receiving the solar rays on a static fixed powerprism, utilizing the static fixed power prism to steer the solar rays ina one direction, and utilizing the electro-optic prism to steer thesolar rays in a different direction. In another embodiment, the methodcan further include receiving the solar rays on a static fixed powerprism, utilizing the static fixed power prism for coarse steering of thelight rays in a direction, and utilizing the electro-optic prism forfine steering of the light rays in the same direction. The lightfocusing element can include a Fresnel lens.

In general, in another aspect, the invention features a method includingreceiving solar rays as the sun moves across the sky. The method furtherincludes applying voltages to an electro-optic prism to control therefractive index of the electro-optic prism and to steer the solar raysin a direction substantially normal to a surface of a light focusingelement. The electro-optic prism includes a layer of electro-opticmaterial with a substantially uniform thickness. The method furtherincludes utilizing the light focusing element to focus the steered solarrays on a photovoltaic device.

Implementations of the invention can include one or more of the featureslisted above as well as the following features. The method can includereceiving the solar rays as the sun moves across the sky from a firstsolar position to a second solar position and then from the second solarposition to a third solar position. The first and third positions arepositions of the sun from which the solar rays from those positions aredirected in directions not substantially normal to the surface of thelight focusing element. The second position is a position of the sunfrom which the solar rays from that position are directed in thedirection substantially normal to the surface of the light focusingelement.

In general, in still another aspect, the invention features a methodincluding receiving solar rays as the sun moves across the sky from afirst solar position to a second solar position and then from the secondsolar position to a third solar position. The first and third positionsare positions of the sun from which solar rays from those positions aredirected in directions not substantially normal to a receiving surfaceof a light focusing element. The second position is a position of thesun from which the solar rays from that position are directed in adirection that is substantially normal to the receiving surface of thelight focusing element. The method further includes controllablysteering the solar rays from the first solar position using anelectro-optic prism to steer the solar rays in the directionsubstantially normal to the receiving surface of the light focusingelement and controllably steering the solar rays from the third solarposition using the electro-optic prism to steer the solar rays in thedirection substantially normal to the receiving surface of the lightfocusing element. The method further includes utilizing the lightfocusing element to focus the steered solar rays on a photovoltaicdevice.

Implementations of the invention can include one or more of thefollowing features. In one embodiment, the electro-optic prism caninclude a first electrode positioned on a first substrate, a secondelectrode positioned on a second substrate, and an electro-opticmaterial positioned between the first electrode and the secondelectrode. The first electrode can include multiple substantiallyparallel linear electrodes. The controllably steering the solar raysusing the electro-optic prism can also include applying a plurality ofvoltages some or all of multiple substantially parallel linearelectrodes to generate a refractive index gradient across theelectro-optic prism. The electro-optic material can be a liquid crystalmaterial.

Implementations of the invention can include one or more of thefollowing.

Implementations of the invention can realize one or more of thefollowing advantages. The light rays can be steered in one or moredirections with an assembly that does not require physical adjustment toaccount for a moving light source. When applied in the context of asolar energy collection assembly, the assembly can be configured tosteer light rays to account for one or both of the sun's east-west andnorth-south movement overhead, without requiring the assembly tophysically move. The solar energy collection assembly can therebyexhibit improved efficiency, reduced size, and a less complicatedmounting structure.

Conventional solar tracking systems can be large, expensive, invitemechanical failure, and be unsightly, potentially deterring people whomight otherwise choose to employ photovoltaic technology as a source ofelectric power. The solar energy collection assemblies described hereinprovide reduced mechanical aspects, decreased cost, and significantlyreduced visual presence.

A light wave impinging with some oblique angle upon a layer ofbirefringent material, such as liquid crystal, can be steered into adifferent angle if an applied electric potential creates a gradient inthe index of refraction (index gradient) in the birefringent material.This is the electro-optic analog of an optical prism; however, unlike aphysical prism, the electric-optic prism can be tuned to refract lightat an arbitrary angle by varying the electric potential and, hence, theindex gradient.

A combination of two or more prisms, each having a different alignmentand/or different electro-optic properties, can be used to achieve bothcoarse and fine solar ray steering. Combining a physically adjustableprism with a non-moving electro-optic prism can provide improved solarray steering in either one or two directions. Solar steering can beimproved by providing a solar energy collection assembly including anelongated photovoltaic element extending in at least one direction,e.g., the east-west direction, and including one or more electro-opticprisms configured to provide solar ray steering in a perpendicular,e.g., north-south direction.

Birefringent nematic liquid crystals require two layers oforthogonally-aligned electro-optic material to act upon bothpolarizations of unpolarized light, such as sunlight. The number ofelectro-optic layers required to steer unpolarized light, e.g., solarrays, can be reduced by using cholesteric liquid crystal as theelectro-optic material.

Lensing, a deleterious effect caused by variations in an electric fieldwithin an electro-optic prism, can be reduced or eliminated usingimplementations described herein. For example, use of a variableresistance electrode can provide a substantially homogeneous electricfield, thereby reducing or eliminating lensing effects.

Light rays incident on a prism can be steered by altering a property ofthe prism, other than the refractive index. Altering the apex angle alsoalters the refraction angle, thereby allowing for controlled lightsteering.

Potentially damaging radiation can be substantially reduced from solarrays incident on a solar energy collection assembly through use of afilter.

Some spectral components of solar radiation that reach a photovoltaicdevice can be outside the absorptive capabilities of light-absorbingmaterial within the device. These photons can be absorbed bychromophores within the prism material, which then emit photons at adifferent wavelength, and can be absorbed by the photovoltaic device.For example, ultra-violet photons included in solar rays can beconverted into visible photons absorbable by a photovoltaic cell.

A particular advantage of the light steering assemblies described hereinis that they can be used to steer solar light rays in a wider range ofincidence angles than conventional steering optics, such as isosceles orequilateral prisms. These conventional components suffer from reflectionlosses, including total internal reflection, when light incident upon areceiving face of the prism enters at oblique angles. The loss can be asignificant factor in photovoltaic systems. The implementationsdescribed herein can overcome this problem by using patterned electrodesto create a refractive index gradient within a substantially flatelectro-optic material. The generated index gradient within the materialis the analog of a traditional optical prism element, e.g., a glassprism, in that light bends as it travels through the material at anangle controlled by the magnitude of the gradient. A distinct advantageof the methods and articles described herein is that the receivingsurface of the electro-optic prism does not need to be adjusted tocompensate for oblique incidence angles, as described below.

Each electrode within the electro-optic material can receive anindependently-controlled voltage, and an index gradient can be createdwithin the electro-optic material in a preferred direction. Theelectro-optic prism can therefore refract incident light rays for manyincidence angles (along a particular planar axis) by controlling thevoltage applied to the electrodes. This is particularly useful forreceiving light rays from a moving source, such as from the sun. As thesun rises in the east, the index gradient can be set, by virtue of theapplied electric fields, such that incident light rays will be steeredtoward a light focusing element and/or photovoltaic surface such thatthe rays enter perpendicular to the light focusing element surface. Asthe sun moves toward its zenith (i.e., solar noon) the index gradientcan be changed to compensate for the movement. When the sun's positionis such that it substantially normal to the flat surface of theelectro-optic prism (i.e., solar noon), the sun's rays may pass directlythrough the material by simply turning off the applied electric field,thereby removing the index gradient. Upon westerly movement of the sun,the index gradient direction may be re-applied, reversed from that whenthe sun was rising from the east. For example, referring to FIGS. 2B-D,when the sun rises in the east and continues to its zenith, the voltagesapplied to electrodes 210 a through 210 f may increase from 210 a to 210f. This particular arrangement may properly refract light rays to areceiving photovoltaic surface during this time period. When the suncontinues from its zenith towards the west, the voltages applied to theelectrodes may now increase from 210 f to 210 a, the reverse of that forthe previous time period. This has the effect of reversing direction ofthe index gradient, and therefore the acceptable incidence angle, andallows solar rays to be steered effectively during the entire course ofa day.

The details of one or more implementations of the invention are setforth in the accompanying drawings and the description below. Otherfeatures, objects, and advantages of the invention will be apparent fromthe description and drawings, and from the claims.

DESCRIPTION OF DRAWINGS

The foregoing summary as well as the following detailed description ofthe preferred implementation of the invention will be better understoodwhen read in conjunction with the appended drawings. It should beunderstood, however, that the invention is not limited to the precisearrangements and instrumentalities shown herein. The components in thedrawings are not necessarily to scale, emphasis instead being placedupon clearly illustrating the principles of the present invention.

FIG. 1 shows a schematic representation of a simplified solar energycollection assembly.

FIGS. 2A-E show schematic representations of solar energy collectionassemblies including electro-optic prisms.

FIG. 3 shows a cross-sectional view of a schematic representation of anelectro-optic prism/light focusing element assembly.

FIG. 4 shows a cross-sectional view of a schematic representation of analternative implementation of an electro-optic prism/light focusingelement assembly.

FIG. 5 shows a cross-sectional view of a schematic representation of analternative implementation of an electro-optic prism/light focusingelement assembly.

FIG. 6 shows a cross-sectional view of a schematic representation of aprism/light focusing element assembly.

FIG. 7 shows a cross-sectional view of a schematic representation of adynamic fixed-power electro-optic prism.

FIG. 8 shows a cross-sectional view of a schematic representation of analternative implementation of a prism/light focusing element assembly.

FIGS. 9A-B show a schematic representation of a light directing assemblyincluding an adjuster and an electro-optic prism/light focusing elementassembly.

FIG. 10 shows a schematic representation of an elongated solarcollecting system positioned on a roof.

FIG. 11 shows a schematic representation of an electro-optic prism/lightfocusing element assembly.

FIGS. 12A-B show cross-sectional views of a schematic representation ofan implementation of a dynamic electro-optic prism.

FIG. 13 shows a cross-sectional view of a schematic representation of anelectro-optic prism exhibiting a lensing effect.

FIG. 14 shows a cross-sectional view of a schematic representation of adynamic electro-optic prism including discrete patterned electrodes.

FIG. 15 shows a cross-sectional view of a schematic representation of analternative implementation of a dynamic electro-optic prism including avariable resistance electrode.

FIGS. 16A-B show schematic representations of a variable-apex angleprism.

FIG. 17 shows a schematic representation of an alternativeimplementation of a variable-apex angle prism.

FIG. 18 shows a schematic representation of a variable-refractiveindex/variable-apex angle prism.

FIG. 19 is a schematic representation of a prism/light focusing elementassembly including an infrared filter.

FIGS. 20A-B are schematic representations showing light directingsystems, including photovoltaic cells with different absorptionproperties.

FIGS. 21A-B show cross-sectional views of schematic representations ofan electro-optic prism including a photon conversion material.

FIG. 22 shows a block diagram representing a system including a solarpowered Stirling engine.

Like reference symbols in the various drawings indicate like elements.

DETAILED DESCRIPTION

Assemblies and techniques are described to steer light rays, includingartificial or naturally occurring light. One application where steeringlight rays has beneficial effects is in the context of solar energycollection. For illustrative purposes, the assemblies and techniquesshall be described in the context of solar rays, however, it should beunderstood that the assemblies and techniques can be applied in othercontexts and to other light sources. The solar energy collectionapplication described herein is but one implementation.

To reduce the cost of manufacturing photovoltaic systems, the amount ofphotovoltaic material required is preferably minimized. Concentratingcaptured solar rays onto a photovoltaic cell is one technique formaximizing solar energy collection efficiency, as more sunlight impingeson the photovoltaic cell than would otherwise impinge on its surfacearea. As described above, conventional solar concentrating arraysgenerally require adjusting the position of a solar energy collectionassembly to track the position of the sun. The assemblies and techniquesdescribed herein to steer and concentrate light rays provide forconfigurations that minimize or eliminate physical adjustment, i.e.,pointing, of the solar energy collection assembly.

Referring to FIG. 1, a schematic drawing shows a point light source,i.e., the sun 110, which emits a broad spectrum of electromagneticradiation (solar rays) 120. The sun 110 continuously travels relative toa terrestrial position, such as the location of a photovoltaic cell 170.A light focusing element 140 can receive the solar rays 120 and focusthem toward the photovoltaic cell 170 (positioned along the optical axis145 of the light focusing element 140), thereby concentrating the amountof solar radiation that would otherwise have impinged on thephotovoltaic cell 170. To be most effective, however, the solar rays 120should impinge on a receiving surface 142 of the light focusing element140 at an approximate 90° angle. That is, to obtain optimal focusingconditions, the point source lies at a point along the optical axis 145of the light focusing element 140. The optical axis 145 of the lightfocusing element 140 is generally an axis of rotational symmetry aboutthe light focusing element 140.

The optical axis 145 in most cases is the axis which, given a pointlight source at a point along the axis 145, would focus or image thelight source with a minimum of spherical or chromatic aberrations orcoma. If the solar rays 120 impinge on the light focusing element 140 atan angle, other than normal, a significant portion of the solar rays 120can be refracted away from the absorbing, or active area, of thephotovoltaic cell 170, dramatically decreasing the light intensity atthe photovoltaic cell 170. The reduction in light intensity has a directbearing on the overall efficiency of solar energy collection.

A light-steering mechanism 150 can steer incoming solar rays 120, suchthat solar rays 120 exiting the light-steering mechanism 150 areincident on the receiving surface 142 of the light focusing element 140approximately normal to the receiving surface 142. The light focusingelement 140 can thereby focus a maximum of the solar rays 120 on thephotovoltaic cell 170.

In one implementation, the light-steering mechanism 150 includes anelectro-optic material configured to direct solar light rays 120 thatpass through the light-steering mechanism 150 by means of opticalrefraction and/or diffraction. The amount of solar light ray steeringrequired, such that light impinges on the receiving surface 142 atnormal incidence, depends on the refractive index of the electro-opticmaterial and the size and shape of optical structures included in thelight steering mechanism 150, which in turn can vary with an electricpotential applied to the material.

Referring to FIG. 2A, in this implementation, the light-steeringmechanism 150 is an electro-optic prism 202. The electro-optic prism 202can include multiple, individual electrodes 210 on a first substrate 220and a reference electrode (e.g., a ground electrode) 230 on a secondsubstrate 240. An electro-optic material 250 of substantially uniformthickness is positioned between the electrodes 210 and 230. In oneimplementation, the electro-optic material 250 can be liquid crystal. Inone implementation, the electrodes 210 and 230 are transparentelectrodes, for example, formed of indium tin oxide.

Applying voltages to the electrodes 210 generates an electric field inthe electro-optic material 250, causing polar molecules therein torotate in the direction of the applied electric field. In someimplementations, the reference electrode 230 is electrical ground. Bycontrolling the voltages to the individual electrodes 210, a gradient inthe refractive index (“index gradient”) of the electro-optic material250 can be created. The index gradient is controlled in accordance withthe angle of incident solar rays 207, which can be in accordance withthe position of the sun relative to the surface 205 of substrate 220. Asthe sun moves, i.e., the angle θ in FIG. 2A changes, the index gradientcan be controllably modified, such that the incident solar rays 207 aresteered from their angle of incidence θ so as to exit the bottom surface242 of the substrate 240 substantially normal to a receiving surface 142of the light focusing element 140. The solar rays 207 are thereforeincident at an approximate 90° angle on the receiving surface 142 andcan thereby properly focused toward the photovoltaic cell 170.

FIGS. 2B-D illustrate an implementation where solar rays 207 are steeredthroughout the course of a day by a light steering mechanism of the typedescribed above. Light rays 207 can be steered such that they impinge onthe light focusing element 140 substantially normal to the receivingsurface 142, so that the solar rays 207 can be substantially focused toa photovoltaic 170. In FIG. 2B, solar rays 207 impinge on a receivingsurface 205 of a first transparent substrate 220 at an angle θ withrespect to the receiving surface 205 of the first substrate 220. InFIGS. 2B-D, the axis of angle θ is at the intersection of solar ray 207and the receiving surface 205 of the substrate 200; θ=0° when the solarray 207 is parallel with the receiving surface 205 and increases to theincidence angle of the solar ray 207 when the solar ray 207 impingesnon-parallel, as indicated in FIG. 2B. Such is the situation, forexample, when the sun rises from the east, from the perspective of astationary viewer in the northern hemisphere of the earth, lookingsouth. A series of linear, patterned, transparent electrode strips 210a, 210 b, 210 c, 210 d, 210 e, and 210 f can be formed on the substrate220, such that the long axes of the electrodes are substantiallyparallel. An electric field can be applied to an electro-optic material250 by applying voltages to the electrodes 210 a-f, wherein thereference electrode 230, formed on the substrate 240, is electricalground.

An index gradient can be created in the electro-optic material 250 thatbends the solar rays 207 an angle φ as shown in FIGS. 2B-D, by applyingsuccessively increasing or decreasing voltages to electrodes 210 a, 210b, 210 c, 210 d, 210 e, and 210 f. The order of increasing or decreasingvoltage applied to electrodes 210 a-f can depend on the incidence angleof the solar rays 207, and how much refraction is necessary to bend thesolar rays 207 to their target (i.e., the photovoltaic 170). In FIG. 2B,the order of increasing voltage applied to the electrodes 210 a-f canincrease in the order: 210 a, 210 b, 210 c, 210 d, 210 e, and 210 f forthe incidence angle shown. In this implementation, the spatial gradientin index of refraction created in the material 250 is controllable fromone side of the electro-optic material 250 (e.g., near electrode 210 a)to the other (e.g., near electrode 210 f), due to the electric fieldscreated between each of the electrodes 210 a-f and the referenceelectrode 230.

The electric field gradient (and therefore the index gradient) isexemplified in FIG. 2B as arrows 252 between the electrodes 210 a-f andthe reference electrode 230. In this example, the strength of theelectric field is indicated by the width of the arrow, where largerarrows indicate higher electric field. The magnitude of the electricfield at each location (each arrow 252) can be governed by the voltageapplied to electrodes 210 a-f. The electro-optic prism 202 in FIG. 2A isthe electro-optical analog of a conventional (e.g. triangular glass orother optical material) prism. The solar rays 207 encountering the indexgradient at an angle θ are refracted at an angle φ as shown in FIG. 2B;the magnitude of the index gradient can be controlled via the appliedvoltages to the electrodes 210 a-f, such that the solar rays 207 impingesubstantially normal on the surface of light focusing element 140.

As the sun moves to a position substantially normal to the surface ofthe substrate 220 (thereby increasing the angle θ to substantially 90°),as shown in FIG. 2C, the index gradient can gradually decrease inmagnitude by applying appropriate voltages to the electrodes 210 a-f. Inthis circumstance the solar rays 207 can propagate substantially free ofangular steering, such that they impinge normal to the receiving surface142 of the light focusing element 140.

FIG. 2D illustrates the reverse process as shown in FIG. 2B, whichoccurs as the sun continues its course across the sky. Now, the voltagesapplied to electrodes 210 a-f can increase in the order: 210 f, 210 e,210 d, 210 c, 210 b, and 210 a. This steers the solar rays 207 an angleφ and can cause the solar rays 207 to impinge substantially normal tothe receiving surface 142 of light focusing element 140.

FIGS. 2B-D illustrate how the electro-optic prism 202 can effectivelycapture solar radiation at a wide range of incidence angles (O) withoutnecessitating angular adjustment of the receiving surface 205 of thefirst substrate 220, or other optical components contained within theelectro-optic prism 202. By this virtue, referring back to FIG. 1,together, the light steering assembly 150, light focusing element 140,and photovoltaic 170 can remain stationary, yet still capture solar rays120 throughout the day. This is unlike the conventional solarconcentrating systems that necessitate physical movement of thecomponents such that they are always facing the sun.

Liquid crystal molecules have a long axis (usually substantiallyparallel to their polar axis) that may be set in a selected orientation,i.e., the orientation that the liquid crystal molecules will assumeunder zero applied electric field, by “brushing” one or more alignmentlayers (for example, a layer of polyamide). Applying an alignment layeraligns the long axes of the liquid crystal molecules near the adjoiningsurfaces of the liquid crystal layer (i.e., top and bottom of the liquidcrystal layer) under zero external field conditions, and subsequentlyaligns the liquid crystal molecules throughout the volume of thematerial. The process of aligning the liquid crystal moleculesthroughout creates birefringence in the liquid crystal material 250.This effect is well known, and arises out of the difference in whichparallel and perpendicular polarization components of light travelthrough the liquid crystal with respect to the long (or polar) axis ofthe molecules. In the absence of an applied electric field, lighttraveling through the liquid crystal (for a given polarization) isprimarily steered in a direction governed by the orientation of theliquid crystal molecules, which should be parallel with the alignmentlayer. Light polarized orthogonal to the liquid crystal director(generally the direction of the long axis of the liquid crystalmolecules when they are aligned) experiences substantially no change inrefractive index as it passes through the liquid crystal. In most cases,the preferred orientation of the director (when no field is applied) isperpendicular to the electric field, when created.

FIG. 2E shows an exploded view of one implementation of a light steeringmechanism 295 configured to steer solar rays 207 (propagating in a plane250) incident on a first substrate 253. The substrate 253 can betransparent and can have attached thereto a series of linear transparentelectrode strips 259 oriented in a selected direction, in this example,along the indicated x-axis. A top liquid crystal alignment layer 262 isapplied to the substrate 253/electrode 259 surface and brushed in aselected direction (in this example the y direction), which orients alayer of liquid crystal 265 in the same direction. A second, bottomliquid crystal alignment layer 268 is brushed in the same direction asthe top liquid crystal alignment layer 262, to ensure total and rapidliquid crystal alignment (under zero externally-applied electric field).

The electrode 271 is supported by a second substrate 274, which can besubstantially transparent. A layer of linear electrodes 277 similar to259 is attached to a lower surface of the substrate 274. In contact withthe substrate 274/electrodes 277 surface is a brushed liquid crystalalignment layer 280 that can be perpendicular to the direction of theliquid crystal alignment layers 262 and 268. The brushed liquid crystalalignment layers 280 and 286 form the top and bottom layers respectivelyof a liquid crystal layer 283. In this case, the direction of the liquidcrystal molecules included in the liquid crystal layer 283 is orthogonalto the liquid crystal molecules included in the liquid crystal layer265. A bottom electrode 289 is supported by a transparent substrate 291and is in contact with the bottom liquid crystal alignment layer 286.

The light steering mechanism 295 shown can steer an unpolarized lightray 207 that impinges on the surface 254 of the substrate 253 at anangle, such that the light ray 207 exits the bottom substrate 291substantially normal, as shown. As it is illustrated in FIG. 2E, thelight steering mechanism 295 only steers light in one direction, thatbeing orthogonal to the direction of the long axis of the electrodes 259and 277. Light rays 207 with polarization vectors orthogonal to thefirst liquid crystal layer 265 pass through the layer 265 unchanged indirection, while those with some degree of parallelism with the liquidcrystal layer 265 undergo some degree of refraction due to the indexgradient. The orthogonal rays can be refracted at the second,orthogonally-aligned liquid crystal layer 283 (with respect to the firstliquid crystal layer 265).

If the light rays 207 impinge normal to the receiving surface 254 of thesubstrate 253, the electrodes can be turned off, and light will passstraight through, emerging normal to the bottom substrate 291.

To allow for two-axis light ray steering, the light steering assembly295 can be cloned, placing one light steering assembly 295 on top of theother, such that the direction of the long axes of the patternedelectrodes 259, 277 in the light steering mechanism 295 areperpendicular to the long axes of the linear electrodes included in thesecond light steering mechanism. As light rays are steered orthogonal tothe long axes of the linear electrodes 259, 277, unpolarized light raysteering in any direction can be accomplished by this approach.

An embodiment of an electro-optic prism can include, for nematic liquidcrystal, all or some of the elements in FIG. 2E. An embodiment of anelectro-optic prism can include, for cholesteric liquid crystal, all orsome of a substrate 253, electrodes 259, liquid crystal alignment layer262, liquid crystal layer 265, liquid crystal alignment layer 268,electrode 271, and substrate 274. For electro-optic prisms usingcholesteric liquid crystal, a second layer of orthogonally-alignedliquid crystal is not necessary to steer light in one direction (as isshown for the light steering mechanism 295 in FIG. 2E), but may be usedin some situations, since an index gradient within a cholesteric liquidcrystal layer can refract unpolarized light.

In one implementation, a solar energy collection assembly, such as thatdescribed in reference to FIGS. 2A-E above, can use a portion of thecollected solar energy for providing the voltages applied to theelectro-optic material 250.

Because optical switching speed is not a significant factor in solarsteering applications, i.e., the speed at which the liquid crystalmolecules align under the influence of the applied electric field,thicker layers of electro-optic material 250 as compared to layers usedin other applications can be desirable, as a thicker layer allows for agreater optical phase delay, making larger angular deflections possible.

Dynamic electro-optic prisms and static prisms described herein can beof either a refractive or diffractive nature, depending on their designand construction, and the implementations described may include eitherprism type. A difference between the two is that a refractive prismsteers light using structures (e.g., electrodes) of a relatively largesize compared to the wavelength of light, while diffractive structuressteer light using structures of a relatively comparable size to thewavelength of light. The behavior of refractive devices can beadequately described using Snell's law, while the wave nature of lightis used to describe the behavior of diffractive devices.

Referring again to FIG. 2A, an electric field is created in theelectro-optic material 250 when a voltage is applied to the electrodes210, and the electrode 230 is a ground electrode. The electrodes 210 canbe linear strips of transparent conducting material. The linearelectrodes 210 can be formed using any convenient technique, forexample, by photolithography, chemical etching, and the like. The groundelectrode 230 can also be a transparent electrode, and in oneimplementation can be similarly constructed of linear strips ofconducting material, or in another implementation, can be a contiguousplanar material. In the latter case, the electrodes may be formed bytechniques known by those skilled in the art of making planartransparent electrodes, such as by chemical vapor deposition (CVD),sputtering, spin-coating, and the like. In one implementation, theelectrodes 210 and 230 are formed from indium tin oxide.

When refraction of incident light rays 207 is desired, such as thatshown in FIG. 2A, it is desirable to space the linear strips oftransparent electrodes 210 a distance that minimizes diffraction of thelight rays 207. Diffractive effects become more prominent when thespacing of a gradient approaches the wavelength of incident light. Inone implementation, such as that shown for FIG. 2A, the spacing of theelectrodes 210 is on the order of three to five microns apart, and thewidth of each electrode (e.g., each linear electrode 259 in FIG. 2E) canbe of the same scale. The length of the electrodes 210 can extend to theboundaries of the substrate 220. In one implementation, a length of theelectrodes 210 can be from six to thirty centimeters.

In certain implementations, a contiguous electrode, rather than stripsof individual electrodes, can be used to create the index gradient inthe electro-optic material. For example, a variable resistance electrodecan be used, which is discussed further below. In this case, the indexgradient can be formed by the potential drop from a first end to asecond end when voltage is applied to the first end. The index gradientcan be formed in a selected direction by applying the driving voltage toa selected end of the variable resistance electrode and grounding theother end. In this manner, sunlight from one direction can be refractedin a selected direction by applying the driving voltage to one end ofthe variable-resistance electrode. The end to which the driving voltageis applied is then reversed when light rays are incident from theopposite angle.

In other implementations, a variable-thickness electrode can provide theindex gradient. A variable-thickness electrode will produce a potentialdrop from one end to which the driving voltage is applied due to itsincreasing thickness. The variable-thickness electrode can be placed ona solar ray-receiving surface of a substrate and is substantiallytransparent. A variable-thickness electrode composed of transparentconducting material can be formed on a substrate by various means knownto those skilled in the art, including CVD, dipping, or sputtering.

Light Ray Steering

To employ an electro-optic prism to steer solar rays from their angle ofincidence to a desired orientation, e.g., orthogonal to a receivingsurface of a light focusing element, information about the sun'sposition is required. The sun's position can be used to estimate theangle of incidence, and thereby provide the electro-optic prism with anappropriate index gradient through application of an electric field. Thesun's position can be tracked using any convenient technique, includingprogramming control electronics for the electro-optic prism withpre-determined solar coordinates (i.e., elevation and azimuthal angles)and/or continuous, active tracking of the sun's position using opticaldetectors and associated electronics in a feedback mode.

In one implementation, the amount of solar energy collected by aphotovoltaic cell can be monitored by associated circuitry; theapplication of the electric field to the electro-optic prism can beintegrated into a feedback mechanism. The index gradient of theelectro-optic prism can be continually adjusted to provide maximumenergy absorption by the photovoltaic cell, based on the informationprovided by the photovoltaic cell monitor.

Additionally, as discussed above, the light steering assemblies andtechniques described herein can be used to steer light rays emanatingfrom a light source other than the sun. If the light source is mobile,similar techniques as described above for solar ray tracking can beemployed to track movement of the light source relative to the lightsteering assembly.

Dynamic Variable-Power Electro-Optic Prism

Referring again to FIG. 2A, the applied voltage applied across theelectrodes 210, 230, affects the strength of an electric field generatedin the electro-optic material 250 near each electrode. By independentlycontrolling the electric field strength at each electrode, a refractiveindex gradient can be formed in the electro-optic material 250. Bycontrolling the refractive index of the electro-optic prism, theelectro-optic prismatic effect can be used to steer the solar rays 207.In the implementation shown, the solar rays 207 are steered to normalincidence on the light focusing element 140 as the sun moves overhead,by varying the strength of the electric field and therefore the indexgradient of the electro-optic prism 202.

The arrow between the reference electrode 230 and the light focusingelement 140 does not necessarily imply a physical space between the twoelements; in some implementations the electrode 230 is depositeddirectly upon a surface of the light focusing element 140.

Electro-Optic Materials

In one implementation, the electro-optic material 250 is liquid crystal.The index of refraction of liquid crystal can be altered to a maximumsaturation depending on the applied electric field. If the liquidcrystal layer then experiences a gradient in the refractive index due toa gradient in the electric field, an optical refractive or diffractiveeffect can occur, resulting in a modification of the phase of a lightwavefront. This effect can be used to focus, steer, or correct arbitrarywavefronts, thereby correcting for aberrations due to light propagationthrough the material. In this sense, liquid crystal cells configured asshown in FIG. 2A can be referred to as electro-optic prisms, since theyeffectively steer light a given amount proportional to an induced indexgradient provided by an external voltage.

Prismatic power is generally a measurement of the magnitude of therefraction or diffraction angle that a light ray undergoes by passingthrough (or diffracting in) a prism. In most cases, light undergoes ahigher degree of refraction (more prismatic power) for prisms formed ofmaterials of high dispersion, i.e., optical index.

As discussed, liquid crystals are generally elongated, polar moleculesthat tend to align axially with one another along their longitudinalaxis. This property of liquid crystals can be used to define a bulkdirection of alignment in a liquid crystal device. The direction of thelocal molecular alignment is referred to as a director as describedabove. Due to these alignment properties, nematic liquid crystal is abirefringent material, and to steer unpolarized light, such as sunlight,two liquid crystal layers having orthogonally arranged alignmentdirections are typically used. That is, the direction of alignment ofthe liquid crystal layer in one electro-optic prism is at approximatelya 90° angle to the director of the second liquid crystal layer in thesecond electro-optic prism when no power is applied, as shown in FIG.2E. By way of example only, a suitable liquid crystal is BL037,available from Merck Co., Germany.

To provide the largest possible range of refractive angles, liquidcrystals that exhibit relatively large differences in refractive indexbetween zero electric field and that at saturation (i.e., they arehighly birefringent) can be used, and should display low chromaticdispersion. For example, a preferred range of the change in index ofrefraction provided by a liquid crystal layer can be from approximately0.3 to 0.4. BL037 liquid crystal has an effective range in refractiveindex of 0.28.

In one implementation, a cholesteric liquid crystal material can be usedin an electro-optic prism. Cholesteric liquid crystal exhibitschirality, and the director is not fixed in a single plane, but canrotate upon translation through the material. In certain configurationsa cholesteric liquid crystal layer can be substantially polarizationinsensitive. Accordingly, an electro-optic prism including a singlelayer of cholesteric liquid crystal can be used to steer unpolarizedlight with high efficiency. Reducing the number of layers of liquidcrystal can reduce undesirable transmission loss. A stronger electricfield, hence higher voltages, can be required to rotate the molecules ofa cholesteric liquid crystal as compared to a nematic liquid crystal.However, since a single layer is capable of affecting both lightpolarizations of the solar rays, using cholesteric liquid crystal canstill improve efficiency.

In another implementation, bistable liquid crystal can be used. Thedirector of a bistable liquid crystal has two or more orientations thatcan be induced by application of an electric field and that remain (i.e.they are stable) after the field is removed. The result of bistablestates is that when the electrical power is turned off, the prismaticeffect remains, thereby minimizing the amount of electrical energyneeded for the electro-optic prism.

For example, a certain voltage can be required to align liquid crystalmolecules in an electric field according to their dipole moment. Whenthat voltage is applied to a bi-stable liquid crystal, the liquidcrystal molecules rotate in the field; at that point, the voltage can beturned off and the liquid crystal molecules retain their orientation.This has the benefit of reducing the energy required to keep the liquidcrystal molecules in a particular orientation to affect a given steeringof incoming light rays. This configuration can be particularly useful ina situation where the movement of the point light source is relativelyminor, such as points on the earth near to either geographic pole. Byway of example only, bistable liquid crystals can include surfacestabilized ferroelectric liquid crystals (SSF liquid crystal).

In one implementation, stacked electro-optic prisms can be used wherethe electro-optic materials, i.e., liquid crystal layers 265 and 283 inFIG. 2E, are different, thereby providing different magnitudes ofprismatic power when the index gradient is created. In certainimplementations, a top electro-optic material, e.g., layer 265 canprovide a filtering effect if its light absorption properties aredifferent than that for layer 283. Unwanted or undesirable wavelengthscan then be absorbed by the first layer 265, allowing desiredwavelengths to continue propagating to layer 283, where they are steeredin a preferable direction.

Electro-Optic Prism/Light Focusing Element Assemblies

Referring to FIG. 3, in one implementation, an electro-optic prism(e.g., 202 in FIG. 2A) 302 and a light focusing element 310 can beconstructed monolithically. In this implementation, the light focusingelement 310 is a Fresnel lens. The receiving surface 312 of the Fresnellens 310 can be used as a substrate to support the parallel, linearelectrodes 320. The electro-optic material 314 and a substrate 318supporting the second electrode 316 are positioned on top of theelectrode 320. If additional electro-optic prisms are desired, e.g., asecond prism arranged with the liquid crystal alignment directionorthogonal to a director of the first prism, they can be constructedsimilarly beginning with an electrode being deposited on a upper surfaceof the substrate 318 followed by a liquid crystal layer and anelectrode. The second prism can be positioned above or below the firstprism, e.g., in a stacked arrangement. Note that in FIG. 3, the linearstrips of transparent electrodes 320 are below the planar transparentelectrode 316, the opposite of that shown, for example, in FIG. 2A. Insome implementations, this arrangement can be used and can result in thesame effect on the electro-optic layer 314.

The Fresnel lens 310 can be configured for point or line concentration.For point concentration, the Fresnel lens 310 is a spherical lens andfor line concentration the Fresnel lens is a cylindrical lens.

Referring to FIG. 4, in one implementation a gap 424 is maintainedbetween an electro-optic prism (e.g. 202 in FIG. 2A) 426 and a lightfocusing element 422. The gap 424 can provide air circulation to coolthe electro-optic prism 426. Anti-reflective coatings 430 can be used toreduce reflection losses on the surfaces of the electro-optic prism 426elements and/or the light focusing element 422. In some implementations,an anti-reflective coating can be included on one or more surfaces inthe electro-optic prism and/or light focusing element, whetherconstructed separately or as an assembly, to minimize loss due toreflections. By way of example only, anti-reflective coatings can beplaced on the outermost surface of the device and are fabricated fromone or more layers of refractory oxides (e.g. SiO₂, Al₂O₃, ZrO₂) havinga thickness of approximately ¼ of an optical wavelength. However,anti-reflective coating can be placed at the interface between any twooptical materials whose refractive indices are not equal to helpeliminate reflective losses.

Two-Axis Steering

FIG. 5 shows an implementation of an electro-optic prism/light focusingelement assembly 500 including two dynamic variable-power electro-opticprisms (e.g., 202 in FIG. 2A) 510, 550, overlaid and orthogonallyaligned with respect to the linear electrode long axis direction. Afirst dynamic variable-power electro-optic prism 510 (having electrodes520, which can be planar electrodes, linear electrodes, or a combinationof both) is arranged with the prism base along the y-axis and the seconddynamic variable-power electro-optic prism 550 (having electrodes 570)is arranged with the prism base along the x-axis. This arrangement canprovide for two-axis steering, for example, to allow north-south as wellas east-west steering as has been previously discussed.

In one implementation, solar rays 207 impinge on a receiving surface 507of a first electro-optic prism 510 and are refracted or diffracted at anangle to compensate for the north-south angular deviation from normalwith respect to the receiving surface 505 of the light focusing element580. The refracted or diffracted solar rays 207 next encounter thesecond electro-optic prism 550, wherein the second prism's electrodes570 are aligned orthogonal to the first prism's electrodes 520. Thesolar rays 207 are now affected by the second electro-optic prism suchthat an angular correction is made for east-west angular deviation. Thesolar rays 207 now continue and impinge on a receiving surface 505 ofthe light focusing element 580 at a substantially 90 degree angle to thereceiving surface 505 of the light focusing element 580.

In one implementation, each of the two dynamic variable-powerelectro-optic prisms 510, 550 shown in FIG. 5 use nematic liquid crystalas the electro-optic material. Accordingly, to account for theunpolarized nature of sunlight, each of prisms 510 and 550 can includetwo nematic liquid crystal layers in each of the electro-optic materiallayers 555, 565 having orthogonally arranged directors. In anotherimplementation, each dynamic variable-power electro-optic prism 510, 550uses a single layer of cholesteric liquid crystal as the electro-opticmaterial 555, 565, respectively.

Referring to FIG. 6, another implementation of an assembly 600 that canprovide two-axis light steering is shown. In this implementation, adynamic variable-power electro-optic prism (e.g., 202 in FIG. 2A) 630 isused in combination with at least one static fixed-power prism 610. Inone implementation, the dynamic variable-power electro-optic prism 630and the static fixed-power prism 610 are arranged such that the prismssteer solar rays 640 in orthogonal directions. For example, north-southsteering can be performed manually by periodic seasonal adjustment ofthe static fixed-power prism 610, and east-west steering can beperformed with the dynamic variable-power electro-optic prism 630, ashas been described above for diurnal adjustment. The assembly 600 caninclude parallel, linear electrodes to generate an index gradient as wasdescribed for the electro-optic prism 202 in FIG. 2A.

In another implementation, the dynamic variable-power electro-opticprism 630 and the static fixed-power prism 610 are arranged such thatthe prisms steer solar rays in the same direction. The staticfixed-power prism 610 can be used for coarse steering and the dynamicvariable power electro-optic prism 630 can be used for fine steering.

In one implementation, the static fixed-power prism 610 is aconventional refractive/diffractive optical element, such as a glassprism, mounted upon a mechanism that provides support and angularadjustment of the prism 610. “Glass” can encompass any of the well-knownmaterials used in the art for refracting or diffracting light, such as“quartz glass,” SF10, liquid crystallite, etc.

In addition to layering dynamic variable-power electro-optic prisms toachieve two-axis light steering, the prisms can be layered to provide alarger, incrementally additive prismatic power when each layer isactivated electrically (i.e., “turned on”). The combined dynamicvariable-power electro-optic prisms can increase or decrease theiroverall prismatic power as required, effecting the desired angular solarray steering.

In some implementations, it may be advantageous to combine electro-opticray steering with a fixed deflection component, for example, the staticfixed-power prism 610 shown in FIG. 6. Thus, various combinations ofdynamic variable-power electro-optic prisms and static fixed-powerprisms can be used to reduce the required dynamic angular range of theelectro-optic prisms.

Dynamic Fixed-Power Electro-Optic Prism

Referring to FIG. 7, a variation of the dynamic variable-powerelectro-optic prism described above for FIG. 6 is the dynamicfixed-power electro-optic prism 700. In this implementation, a staticfixed-power prism (or array of prisms) 710 is positioned in contact witha layer of electro-optic material, e.g., a liquid crystal layer 720.Electrodes 730, 735 are included on opposing surfaces of the liquidcrystal layer 720 to apply an electric field, as described above. In oneimplementation, one of the electrodes is electrical ground, e.g.,electrode 735.

The dynamic fixed-power prism 700 has two modes: an “on” mode and an“off” mode. That is, in the “on” mode, a fixed electric potential isapplied across the electrodes 730, 735, generating an electric field inthe liquid crystal layer 720, resulting in light being steered in afirst direction. In the “off” mode, no electric potential is appliedacross the electrodes 730, 735, resulting in light being steered in asecond direction, or not steered at all if the liquid crystal layer 720and the fixed-power prism 710 are index-matched. The voltage applied tothe electrodes 730, 735 is either on or off, resulting in light beingsteered in one of two fixed directions (or allowed to propagate straightthrough in the index-matched case), thus the term “dynamic fixed-powerprism.”

The liquid crystal layer 720 can be index-matched in either the “on” or“off” mode to the material forming the static fixed-power prism 710.When index-matched, there is no prismatic power. In the mismatched mode,i.e., the refractive indices of the liquid crystal layer 720 and staticfixed-power prism 710 are different; the dynamic fixed-powerelectro-optic prism diffracts/refracts light at a fixed angle determinedby the blaze angle of the static fixed-power prism 710. In oneimplementation, a pair of dynamic fixed-power electro-optic prisms areoppositely positioned in a stacked arrangement to provide a grossangular steering correction for two quadrants of the sky, e.g., toprovide steering of solar rays emanating from both the east and thewest. The electrodes 730, 735 in this implementation can be contiguous,as they are only used to provide a change in the index of refraction ofthe liquid crystal layer 720.

In another implementation, a dynamic variable-power electro-optic prism(e.g., 202 in FIG. 2A) can be added to a stack of dynamic fixed-powerelectro-optic prisms 700, where the dynamic variable-power electro-opticprism provides “fine tuning” of light ray steering, in addition to thecoarse light ray steering provided by the dynamic static-power electrooptic prisms 700.

In an implementation using cholesteric liquid crystal as theelectro-optic material in the various prisms, a stacked assemblyincludes at least three electro-optic prisms: one dynamic variable-powerelectro-optic prism (e.g., 202 in FIG. 2A) and two dynamic fixed-powerelectro-optic prisms 700. Only one dynamic variable-power electro-opticprism is required, since the dynamic variable-power electro-optic prismcan be provided with voltages to refract solar rays from two directions,e.g., from either east or west.

Referring to FIG. 8, an implementation including a dynamicvariable-power electro-optic prism (e.g., 202 in FIG. 2A) 802 incombination with two dynamic fixed-power electro-optic prisms (e.g., 700in FIG. 7) 804, 806 is shown. In this implementation, the electro-opticmaterial for each prism can be cholesteric liquid crystal. The dynamicvariable-power electro-optic prism 802 can be fabricated monolithicallywith the dual-etched dynamic fixed-power electro-optic prisms 804, 806.

The dynamic variable-power electro-optic prism 802 can include a driveelectrode 810 affixed to a substrate 825 and a reference electrode 820affixed on an electrode substrate 830. A liquid crystal layer 835 can bepositioned between the reference electrode 820 and the drive electrode810.

A drive electrode 840 for the first dynamic fixed-power electro-opticprism 804 can be formed on the opposite side of the electrode substrate830 as the electrode 820 for the dynamic variable-power electro-opticprism 802. A layer of liquid crystal 845 is positioned on a staticfixed-power prism 850, which itself is positioned on a referenceelectrode 855 for the first dynamic fixed-power electro-optic prism 804.

A second dynamic fixed-power electro-optic prism 806 shares thereference electrode 855 with the first dynamic fixed-power electro-opticprism 804. A static fixed-power prism 860 is positioned under thereference electrode 855 and adjacent a liquid crystal layer 865. Asecond drive electrode 870 is positioned thereunder. The electrodes 870and 855 can be contiguous to solely provide a change in the refractiveindex of the liquid crystal layer 865.

The above described elements can be supported by a light focusingelement 880, for example, a Fresnel lens.

In some implementations, one or more additional layers of electro-opticprisms can be used to produce a desired range of solar ray steering. Insome implementations, it can be desirable that the maximum refractionmagnitude of a dynamic variable-power electro-optic prism be equal tothe magnitude of the largest dynamic fixed-power electro-optic prism.

Combined Physical and Light Steering Adjustment

In one implementation, the angular physical orientation of the solarenergy collection assembly is adjusted using either a manual orautomatic adjuster, in combination with light steering using one or moreelectro-optic prisms. The one or more electro-optic prisms can bedynamic variable-power electro-optic prisms, dynamic fixed-powerelectro-optic prisms, or a combination of both. A mechanical tracker canbe used to provide some angular physical orientation adjustment. Themechanical tracker does not necessarily need to achieve high accuracyand can be of reduced cost. In one implementation, the mechanicaladjuster provides coarse solar ray tracking and the one or moreelectro-optic prisms provide fine solar ray steering. In anotherimplementation, the adjuster provides solar ray tracking along one axis,for example, in a north-south direction, and can be adjusted seasonally,and the one or more electro-optic prisms provide diurnal solar raysteering in an east-west direction.

Referring to FIG. 9A, a schematic representation of one implementationof a system 900 including a dynamic variable-power electro-opticprism/light focusing element assembly (e.g., 202 in FIG. 2A) 905, aphotovoltaic cell 920, and an adjuster 930 are shown. In thisimplementation, the adjuster 930 includes a rotatable support that, forexample, can tilt the assembly 905 in elevation, an angle β. Theelevation angle β can be adjusted, for example, to account for seasonalvariation in the elevation of the sun relative to the horizon, for aterrestrial observer. For example, the path 915 of the sun is shown forone part of a year where the elevation angle β of the sun 901 is low.The elevation angle β can be set using the adjuster 930 such that theassembly 905 is pointing at the sun 901, with respect to the sun'selevation. The variable-power electro-optic prism component cancompensate for the daily travel of the sun 901 in the daily azimuthal(e.g., east-west) direction, directing light rays impinging on theassembly to the photovoltaic 920, as has been discussed above. At adifferent time of year, as illustrated in FIG. 9B, the sun's elevationcan be higher (as shown for path 917); at this time, the tilt angle β ofthe assembly 905 can be re-positioned to compensate for the increase inelevation of the sun relative to the horizon.

In another implementation, the axes for each steering mechanism can bereversed, with the mechanical steering adjusting for diurnal sunposition. Any suitable mechanism to rotate an electro-optic prism 910supporting assembly 905 can be used, for example, a gear assembly 940 asshown, which can be driven by a motor (not shown) or a manual hand crank950 as shown. The implementation shown is a simplified system forillustrative purposes, and other configurations of physical trackingdevices can be used.

Elongated Solar Energy Collection Assembly

In one implementation, an elongated strip of photovoltaic element can beused instead of a round or square element. In this implementation, thesolar energy collection assembly can include several elongated Fresnellenses with cylindrical focusing properties (as compared to a number ofindividual spherical-focus Fresnel lenses), the lenses arranged inseparate rows or columns which are parallel to one another. One or moreelectro-optic prisms, such as a dynamic variable-power electro-opticprism, a dynamic fixed-power electro-optic prism or a combinationthereof, receive solar rays and steer them in an orthogonal direction tothe receiving surfaces of the Fresnel lenses. One or more elongatedphotovoltaic elements are positioned beneath the Fresnel lenses andreceive concentrated solar rays therefrom.

In one implementation, the need for solar ray tracking and steering inone direction can be eliminated if the elongated solar energy collectionassembly is axially aligned in the direction. For example, referring toFIG. 10, the solar energy collection assembly 1000 is positioned alongthe length of a roof 1010 of a building 1020. The roof 1010 runs in aneast-west direction, and the solar energy collection assembly 1000 isthereby axially aligned in the east-west direction. Accordingly, as thesun passes over the building 1020 in the course of a day, at least someportion of an elongated photovoltaic element included within theassembly 1000 is exposed to and receives solar rays. Accordingly, lightsteering in the east-west direction can be eliminated. The one or moreelectro-optic prisms can be used to correct for seasonal variations inthe north-south direction.

Electro-Optic Prism/Mirror Assembly

Referring to FIG. 11, a solar energy collection assembly 1140 is shownfor collecting solar energy emanating from the sun 1105. In someimplementations, a light focusing element 1120 included in a solarenergy collection assembly can be a curved mirror, where the mirrorfocuses light rays 1107 onto a photovoltaic 1130 after being properlysteered by an electro-optic prism 1110, e.g., electro-optic prism 202 inFIG. 2A. The light focusing element 1120 can be positioned in opticalcommunication with an electro-optic prism 1110. In some implementations,the electro-optic prism 1110 can be configured according to the variousconfigurations described herein. Refracted solar rays 207 exiting theelectro-optic prism 1110 are incident on the curved mirrored surface1120 and then concentrated toward the photovoltaic element 1130.

Lensing

Referring to FIGS. 12A and 12B, a cross-sectional view of oneimplementation of a dynamic electro-optic prism 1200 is shown. Thedynamic electro-optic prism 1200 includes an electro-optic material 1220having a substantially triangular cross-section. In one implementation,the electro-optic material 1220 is liquid crystal. The index ofrefraction of the electro-optic material 1220 can be tuned continuouslybetween a minimum and maximum value by applying a selected electricfield strength across the electro-optic material 1220, thereby tuningthe beam deflection angle.

At one extreme, the difference between the refractive indices of theelectro-optic material 1220 and the surrounding medium 1210 is maximizedand an incident light ray undergoes a maximum angular deflection. At theother extreme, the refractive indices of the electro-optic material 1220and surrounding medium 1210 are matched, and an incident light rayundergoes substantially zero deflection, as shown in FIG. 12B.

The difference between the dynamic electro-optic prism shown in FIGS.12A and 12B is the application of an electric potential and theresulting effect on light refraction. The entrance and exit faces of theelectro-optic material 1220 can be coated internally or externally witha thin layer of transparent conductor (e.g., indium tin oxide) to formplanar electrodes 1230 and 1240. As discussed above, when an electricpotential is applied across the two electrodes 1230, 1240, an electricfield is generated internal to the electro-optic material 1220. When theelectro-optic material is liquid crystal, the liquid crystal molecules,which can be initially oriented perpendicular to the electric field,rotate in the direction of the electric field. The higher the voltage,the stronger the electric field intensity, and the greater the change inthe refractive index from the zero-field state. In a solar ray steeringapplication, two such prisms 1200 arranged with the liquid crystalalignment directions orthogonal to one another can be used to steer allof the incoming solar rays to overcome the unpolarized nature ofsunlight.

As discussed, lensing is an effect that can negatively impact the lightsteering performance of an electro-optic prism, such as an electro-opticprism 1200 having the configuration shown in FIG. 12A. If the separationof the electrodes 1230, 1240 is substantially constant, then theelectric field strength within the electro-optic material 1220 issubstantially homogeneous. However, because of the triangularcross-section of the electro-optic material 1220, the separation of theelectrodes 1230, 1240 varies linearly from the apex 1250 to the opposingedge 1260 of the electro-optic material 1220. Because the electric fieldstrength varies across the electro-optic material 1220, the refractiveindex also varies. Referring to FIG. 13, the effect of an inhomogeneouselectric field and therefore a non-linear index gradient across theelectro-optic material 1220 is shown.

In one implementation, the deleterious effects of lensing can besubstantially eliminated by providing a substantially homogeneouselectric field across the electro-optic material 1220, thereby providinga substantially linear index gradient. Referring to FIG. 14, oneimplementation of an electro-optic prism 1400 configured to eliminatelensing is shown. In this implementation, an electrode 1410 provided ona face of the electro-optic material 1450 is patterned instead ofcontiguous. In this implementation, the patterned electrode 1410 isprovided on the entrance face, although in another implementation thepatterned electrode can be provided in the exit face.

The electrode 1410 can be patterned in linear strips 1435, where eachstrip can be individually wired with electrical connections that allow aunique voltage to be applied to each individual electrode, as depictedby V₁, V₂, V₃ . . . V_(N) in FIG. 14. The electric field in the vicinityof an electrode strip 1435 can thereby be controlled to account for thethickness of the electro-optic material 1450 adjacent to the electrodestrip. Accordingly, increased voltages can be applied to the electrodestrips 1435 at the thicker end 1430 of the electro-optic material 1450and a reduced voltage applied toward the thinner end 1440. The additiveeffect of the individual voltages can provide a substantiallyhomogeneous electric field, thereby causing the same amount of molecularrotation across the electro-optic material 1450 and hence asubstantially linear index gradient. The effects of lensing can therebybe substantially eliminated.

In another implementation of an electro-optic prism 1500 shown in FIG.15, one or more variable resistance electrodes 1570 can be used insteadof a patterned electrode, e.g., 1410 in FIG. 14. In this implementation,one end 1520 of the variable resistance electrode 1570 can be held at amaximum required voltage V₂ and the other end 1530 can be held at aminimum required voltage V₁, which in one implementation is electricalground. As current flows between the high potential 1520 and lowpotential 1530 ends of the resistance electrode 1570, the variableresistance of the resistance electrode 1570 dictates the localpotential, and hence the local electric potential applied across theelectro-optic material 1540. Again, by varying the electric potentialapplied to the differing thicknesses of the electro-optic layer 1540, asubstantially homogeneous electric field can be applied resulting in asubstantially linear index gradient.

In one implementation, the variable resistance electrode 1510 isfabricated by providing a layer of a transparent conductor with variablethickness. In another implementation, the variable resistance electrode1510 is formed from a substantially uniformly thick, high-resistancetransparent conductive layer that is patterned in such a manner as toeffectively alter the resistance from one end 1520 to the other end1530.

In one alternative implementation, the variable resistance electrode canbe positioned on an inner surface of a top cover plate that shields theelectro-optic material 1540 from the environment. A space between thecover plate and the entrance face of the electro-optic layer 1540 caninclude air and does not affect the deflection angle of impinging lightrays.

Varying Apex Angle

A prism having a triangular cross-section bends light rays through agiven refraction angle that is primarily dependent upon the wavelengthof the incident light, the index of refraction of the prism material,the apex angle of the prism, and the angle of incidence of the incomingrays. The apex angle is the angle subtended by the entrance and exitfaces of the prism. As already discussed above, varying the refractiveindex of the prism material can provide a dynamic light steering effect.In another implementation, the apex angle can be varied to provide adynamic light steering effect. Light rays can thereby be refracteddynamically without physically altering the prism's orientation.

Referring to FIGS. 16A and 16B, one implementation of a prism assembly1600 having a variable apex angle α is shown. In general, the prism 1600has a variable volume and the apex angle α varies based on variations inthe volume. In this implementation, the prism 1600 can include twotransparent plates 1610 pivotally connected at the apex 1602. The plates1610 can be connected by a pivotal connector 1620, including by way ofexample, a hinge or a living hinge. The orientation of the plates 1610can be nearly vertical, nearly horizontal, or at any intermediate angleα. A third surface 1630 is connected to both plates 1610, forming asubstantially triangular cross-section to the prism cavity 1665. Thethird surface 1630 is configured to expand and contract as the volume ofthe prism cavity 1665 varies. In one implementation, the third surface1630 is an accordion-like configuration, as shown. In anotherimplementation, the third surface 1630 is a flexible membrane.

The prism cavity 1665 is sealed on either end providing a liquid-tightcontainer. The prism cavity 1665 is in fluid communication with a fluidsource 1640, wherein varying the volume of fluid 1650 contained in theprism cavity 1665 varies the volume of the prism cavity 1665 and in turnvaries the apex angle α. In one implementation, the fluid source is areservoir 1640 containing a fluid 1650 connected by a hose 1635 to theprism cavity 1665. A pump 1660 can be used to precisely transfer fluid1650 into and out of the prism cavity 1665.

When the light source 1670 is positioned such that the light rays 1675impinge on the entrance surface 1604 of the prism 1600 at substantiallya 90° angle, the prism cavity 1665 can be substantially drained of thefluid 1650, as shown in FIG. 16A. As the light source 1670 moves (e.g.,the sun moving across the sky) the fluid 1650 can be pumped into theprism cavity 1665 to expand the volume and thereby increase the apexangle α, as shown in FIG. 16B. The increase in apex angle α iscontrolled to provide a controlled dynamic light-steering effect, suchthat the angle of the light rays 1675 exiting the prism 1600 iscontrolled. Examples of the fluid 1650 used in this implementation caninclude any low-viscosity, non-volatile liquid with low opticalabsorption. Fluids 1650 can be any of the materials generally referredto as “index matching fluids” known in the art and commonly used inoptical microscopy applications.

In one implementation, the light rays exiting the prism 1600 can besubstantially orthogonal relative to a receiving surface of a lightfocusing element 1680 positioned to focus light rays on a photovoltaiccell 1690. It may be beneficial to have two such prisms 1600 to providefull sky coverage from sunrise to sunset, as discussed previously.

Referring to FIG. 17, another implementation of a variable apex-angleprism 1700 is shown. The prism 1700 has a similar configuration to theprism 1600 discussed above, however, in this implementation, a flexible,transparent bladder 1710 is included within the variable volume prismcavity 1720. The bladder 1710 allows fluid 1750 to be pumped (such asthrough hose 1735 and pump 1740 system) into and out of the prism cavity1720 from a fluid source, such as a fluid reservoir 1740. The bladdercan be made from any pliable, transparent plastic or polymer withsuitable optical qualities, including low absorption and dispersion.

Combined Variable-Apex Angle and Variable-Refractive Index Prism

To achieve an increased angular range for light-steering, avariable-apex angle design can be combined with a variable-refractiveindex design. Referring to FIG. 18, in this implementation of a dynamicprism 1800, fluid 1850 pumped into and out of the variable volume prismcavity 1820 is a liquid crystal material. The prism plates 1810 supportelectrodes 1830, 1840, such that an electric field can be applied to theliquid crystal 1850. In one implementation, one of the electrodes 1830or 1840 is a variable resistance electrode, as discussed above, toeliminate a lensing effect. One or both of electrodes 1830 and 1840 maybe linear parallel electrode strips, and can haveindividually-controllable voltages applied thereto, as described forelectro-optic prism 202 in FIG. 2A. The electric field strength can bevaried to vary the refractive index in combination with the apex anglebeing varied with the variable volume of the prism cavity 1820,providing controlled light steering of light rays impinging on theentrance face 1860.

Radiation Filtering

In any of the above described implementations, the assemblies can beexposed to significant amounts of solar radiation, particularly in theinfrared portion of the electromagnetic spectrum. Exposure to infraredradiation can cause undesirable heating. To protect against the negativeeffects of infrared radiation, a filter for reflecting, absorbing orotherwise redirecting infrared radiation, while allowing visibleradiation to pass through for the purpose of reaching a photovoltaicdevice, can be employed. The filter can include, by way of example, oneor more of a dichroic mirror, an interference filter, a cut-off filterand a diffraction grating. The filter can be used in conjunction withthe various assemblies described herein, including the dynamicvariable-power electro-optic prism, dynamic fixed-power electro-opticprism and static fixed-power electro-optic prism assemblies described.

Referring to FIG. 19, a cross-sectional view of a schematicrepresentation of a prism/light focusing element assembly 1900 includingan infrared filter 1910 is shown. In this implementation, the infraredfilter 1910 is positioned directly above and in optical communicationwith a dynamic electro-optic prism (e.g., any of the electro-opticprisms discussed above) 1912. Other configurations of prism/lightfocusing element assemblies can be used incorporating an infraredfilter, and the configuration shown is but one example. Moreover, inother implementations a filter can be configured to reduce the effectsof other types of radiation other than or in addition to infraredradiation. For example, in an outer-space application, it may bedesirable to reduce exposure of a light directing system to other typesof potentially damaging radiation or particles.

Dispersive Properties of Prisms

Sunlight is a broadband illumination source. The refraction angle of thedynamic variable-power electro-optic prism can be optimized to steerlight with a wavelength at the peak of the solar visible spectrum to thenormal direction with respect to a receiving surface of a light focusingelement.

All prisms exhibit dispersion. In one implementation, the dispersion canbe maximized and two or more locations in a photovoltaic cell withdifferent absorption properties can be targeted, such that anappropriate wavelength of light impinges on a corresponding location inthe photovoltaic cell, thereby improving absorption and conversionefficiency over that of a single targeted location. Photovoltaicmaterials that absorb different regions of the solar spectrum are wellknown in the art. The solar spectrum is not homogeneous; there are somewavelengths that arrive at terrestrial levels in higher flux thanothers. In some implementations, it is desirable to use photovoltaicmaterials that are more sensitive at those wavelengths, thereby moreefficiently converting light into electrical energy for those particularregions of the solar spectrum.

Referring to FIG. 20A, one implementation of a system 2000 where thedispersive properties of a prism is shown. In this implementation, thesystem 2000 includes an electro-optic prism (e.g., 202 in FIG. 2A) 2010that refracts light from a broadband source, such as the sun 2007. Thedispersive property of the prism 2010 can separate the broadband lightinto discrete wavelength “bands,” indicated by 2015, a prismatic effectwhich is well known. For example, a white-light beam entering atriangular prism separates the white light into a “rainbow” of colors asit exits the prism. A photovoltaic element 2020 includes differentlight-absorbing materials within one or more discrete cells 2030, 2032,2034, 2036, which absorb wavelengths of light in a given range.

The electro-optic prism 2010 can steer incoming light rays 2005 suchthat when the light rays 2005 are subsequently divided into theirconstituent wavelength components 2015 by the prism 2010, the wavelengthcomponents 2015 are directed (by way of the light-steering property ofthe electro-optic prism 2010) to certain cells 2030, 2032, 2034, 2036.For example, cell #1 (2030) may be a photovoltaic material that isefficient at absorbing light in the wavelength range 1000-1600nanometers (nm), but not wavelengths outside of this range. Theelectro-optic prism 2010 can be operated such that the dispersion andlight-steering of the electro-optic prism 2010 directs wavelengthsbetween 1000 nm and 1600 nm substantially toward cell #1 (2030). Otherwavelength bands can be similarly substantially focused on the remainingcells according to the absorption properties of the cells, i.e., cells2032, 2034, and 2036.

Referring to FIG. 20B, another implementation is shown including a lightfocusing element 2060 that directs the dispersed light onto thephotovoltaic element 2020 at an angle substantially normal to thereceiving surface 2025 of the photovoltaic 2020, which includes theaforementioned photovoltaic cells 2030, 2032, 2034, 2036. The lightfocusing element 2060 can reduce the effect to of spectral ‘bleeding’into adjacent cells. For example, referring to FIG. 20A, dispersed raysexit the prism 2010 as substantially a point source 2017. If thedistance from the prism 2010 to the photovoltaic element 2020 is notsuch that component wavelengths are spatially separated, then cells 2030and 2032 can receive photons outside of their design purpose. The lightfocusing element 2060 included in the assembly in FIG. 20B can allowseach dispersed spectral component to be directed substantially normal tothe receiving surface of the photovoltaic element 2020, and also to therespective cell for which absorption will be maximized.

Ultra-Violet to Visible Photon Conversion

The efficiency of a solar energy collection assembly can be improved bycapturing radiation that falls outside the visible spectral region. Forexample, ultra-violet photons included in incoming solar radiation isdown-converted into the visible band. In one implementation, certainchemical phosphors are included in the fluid of a light-steeringmechanism, whether an electro-optic prism, a variable-apex prism or acombination thereof. In another implementation, an additional layerincluding chemical phosphors that optically communicates with thelight-steering mechanism, and/or light focusing element is included.Ultra-violet light is thereby absorbed and converted into visiblephotons, steered normal onto a light focusing element, and concentratedonto a photovoltaic material, increasing the solar energy collectionassembly's efficiency.

Referring to FIGS. 21A and 21B, one implementation of a light-steeringmechanism employing ultra-violet light conversion is shown. In thisexample, the light-steering mechanism 2100 is a dynamic electro-opticprism 2130 as described above in reference to FIG. 13. FIG. 21A showsthe prism 2130 without the inclusion of chemical phosphors to provideultra-violet light conversion. As illustrated, ultraviolet photons 2115incident on the prism 2130 are absorbed by some component of the prism2130. This can arise from the absorption properties of the liquidcrystal, the optical elements, or the electrodes, for example.

Referring now to FIG. 21B, the electro-optic prism 2130 includeschemical phosphors 2120 that can absorb the ultra-violet photons 2115and emit a different frequency photon, generally characterized by theStokes shift of the molecules 2120. The down-converted photons 2140emitted from the electro-optic prism 2130 can be directed toward aphotovoltaic cell via a light focusing element (not shown in FIG. 21B),where the photons 2140 are in a frequency range to be absorbable by aphotovoltaic cell (not shown in FIG. 21B). In general, the phosphorsused in this implementation can include, but are not limited to: organicdyes, inorganic phosphors, semi-conductor phosphors and quantum confinedsemi-conductors, such as nano-crystals, core-shell nano-crystals (aninorganic nano-crystal core surround by a shell of differentsemi-conductor), nanotubes, etc. By way of example only, the commerciallaser dye Rhodamine 590 Chloride can be fluorescent (absorbs UV photonsand emits visible photons) when dissolved in a liquid medium and couldbe added to the electro-active material used in an electro-active prismor the liquid used in a variable apex prism.

The technique of photon conversion described above can be implemented inthe various light-steering mechanisms described herein, includingwithout limitation the dynamic variable-power electro-optic prism,dynamic fixed-power electro-optic prism and static fixed-powerelectro-optic prism assemblies described.

Stirling Engine Application

Stirling engines have been used in conjunction with solar collectors todrive generators to produce electricity. Solar heating is used to drivethe Stirling engine at relatively high efficiency, which then rotates agenerator armature to produce electric power. In one implementation, oneor more electro-optic prisms in any configuration discussed herein forthe purpose of light steering can be used to direct sunlight to asolar-powered Stirling engine, which can eliminate the necessity for amechanical steering system for directing solar energy to the engine.

Referring to FIG. 22, a schematic representation of a system 2200including a solar-powered Stirling engine 2210 is shown. The system 2200includes a solar energy collection assembly 2204 configured to providesolar energy to the Stirling engine 2210. The solar energy collectionassembly 2204 receives solar rays 2202 from the sun. The solar rays 2202impinge on a dynamic electro-optic prism 2206, which can be configuredin accordance with the various implementations described herein. Thesolar rays exit the dynamic electro-optic prism 2206 substantiallynormal to a receiving surface of a light focusing element 2208. Thelight focusing element 2208 focuses the solar rays 2202 toward a heatingelement of the Sterling engine 2210. Electrical power generated from thesolar energy absorbed by the heating element powers the Stirling engine.In another implementation, a large-area array of dynamic electro-opticprisms individually steer light directly onto the absorber of theStirling engine, which can eliminate the need for solar light rayfocusing elements.

A number of implementations of the invention have been described.Nevertheless, it will be understood that various modifications can bemade without departing from the spirit and scope of the invention. Thedevices enabled can be placed on crafts that exit the Earth'satmosphere, such as the Space Shuttle, or Space Station. The activeabsorbing medium can include semiconductors, as are known in the art, orother variants, to include nano-crystals, nano-tubes, and the like.Accordingly, other implementations are within the scope of the followingclaims.

1. A method comprising: (a) receiving solar rays onto a surface of anelectro-optic prism comprising: (i) a first electrode positioned on afirst substrate, wherein the first electrode comprises a plurality ofsubstantially parallel linear electrodes, (ii) a second electrodepositioned on a second substrate, and (iii) an electro-optic materialpositioned between the first electrode and the second electrode; (b)applying a plurality of voltages to at least some of the plurality ofsubstantially parallel linear electrodes to generate a refractive indexgradient across the electro-optic prism; (c) controlling the refractiveindex gradient so that the solar rays exit the electro-optic prism in adirection substantially normal to a light focusing element; and (d)utilizing the light focusing element to focus the solar rays on a solarenergy collector.
 2. The method of claim 1, wherein the solar energycollector comprises a photovoltaic device.
 3. The method of claim 1,wherein the electro-optic material comprises a liquid crystal material.4. The method of claim 3, wherein the liquid crystal material is acholesteric liquid crystal.
 5. The method of claim 3, wherein the liquidcrystal material is a nematic liquid crystal.
 6. The method of claim 1,wherein the electro-optic material positioned between the firstelectrode and the second electrode is of substantially uniformthickness.
 7. The method of claim 1, further comprising: (e) receivingthe solar rays on a static fixed power prism; (f) utilizing the staticfixed power prism to steer the solar rays in a first direction; and (g)utilizing the electro-optic prism to steer the solar rays in a seconddirection.
 8. The method of claim 1, further comprising: (e) receivingthe solar rays on a static fixed power prism; (f) utilizing the staticfixed power prism for coarse steering of the light rays in a firstdirection; (g) utilizing the electro-optic prism for fine steering ofthe light rays in the first direction.
 9. The method of claim 1, whereinthe light focusing element comprises a Fresnel lens.
 10. A methodcomprising: (a) receiving solar rays as the sun moves across the sky;(b) applying voltages to an electro-optic prism to (i) control therefractive index of the electro-optic prism and (ii) steer the solarrays in a direction substantially normal to a surface of a lightfocusing element, wherein the electro-optic prism comprises a layer ofelectro-optic material with a substantially uniform thickness; (c)utilizing the light focusing element to focus the steered solar rays ona photovoltaic device.
 11. The method of claim 10, wherein theelectro-optic material comprises a liquid crystal material.
 12. Themethod of claim 11, wherein the liquid crystal material is a cholestericliquid crystal.
 13. The method of claim 11, wherein the liquid crystalmaterial is a nematic liquid crystal.
 14. The method of claim 10,further comprising: (d) receiving the solar rays on a static fixed powerprism; (e) utilizing the static fixed power prism to steer the solarrays in a first direction; and (f) utilizing the electro-optic prism tosteer the solar rays in a second direction.
 15. The method of claim 10,further comprising: (d) receiving the solar rays on a static fixed powerprism; (e) utilizing the static fixed power prism for coarse steering ofthe light rays in a first direction; and (f) utilizing the electro-opticprism for fine steering of the light rays in the first direction. 16.The method of claim 10, wherein the light focusing element comprises aFresnel lens.
 17. The method of claim 10, wherein said receiving stepcomprises receiving the solar rays as the sun moves across the sky froma first solar position to a second solar position and then from thesecond solar position to a third solar position, and wherein (i) thesolar rays from the first position of the sun and the third position ofthe sun are directed in directions not substantially normal to thesurface of the light focusing element, and (ii) the solar rays from thesecond position of the sun are directed in the direction substantiallynormal to the surface of the light focusing element.
 18. A methodcomprising: (a) receiving solar rays as the sun moves across the skyfrom a first solar position to a second solar position and then from thesecond solar position to a third solar position, wherein (i) the solarrays from the first solar position of the sun and from the third solarposition of the sun are directed in directions not substantially normalto a receiving surface of a light focusing element, and (ii) the solarrays from the second solar position of the sun are directed in adirection that is substantially normal to the receiving surface of thelight focusing element; (b) controllably steering the solar rays fromthe first solar position using an electro-optic prism to steer the solarrays in the direction substantially normal to the receiving surface ofthe light focusing element; (c) controllably steering the solar raysfrom the third solar position using the electro-optic prism to steer thesolar rays in the direction substantially normal to the receivingsurface of the light focusing element; and (d) utilizing the lightfocusing element to focus the steered solar rays on a photovoltaicdevice.
 19. The method of claim 18, wherein: (i) the electro-optic prismcomprises (A) a first electrode positioned on a first substrate, whereinthe first electrode comprises a plurality of substantially parallellinear electrodes, (B) a second electrode positioned on a secondsubstrate, and (C) an electro-optic material positioned between thefirst electrode and the second electrode; and (ii) controllably steeringthe solar rays using the electro-optic prism comprises applying aplurality of voltages to at least some of the plurality of substantiallyparallel linear electrodes to generate a refractive index gradientacross the electro-optic prism.
 20. The method of claim 19, wherein theelectro-optic material comprises a liquid crystal material.